CN101918814A - Method for operating an FTIR spectrometer, and FTIR spectrometer - Google Patents
Method for operating an FTIR spectrometer, and FTIR spectrometer Download PDFInfo
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- CN101918814A CN101918814A CN2008801170089A CN200880117008A CN101918814A CN 101918814 A CN101918814 A CN 101918814A CN 2008801170089 A CN2008801170089 A CN 2008801170089A CN 200880117008 A CN200880117008 A CN 200880117008A CN 101918814 A CN101918814 A CN 101918814A
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- 238000000034 method Methods 0.000 title claims abstract description 27
- 238000005033 Fourier transform infrared spectroscopy Methods 0.000 title claims description 21
- 239000007789 gas Substances 0.000 claims abstract description 131
- 238000001228 spectrum Methods 0.000 claims abstract description 23
- 238000000862 absorption spectrum Methods 0.000 claims abstract 2
- 238000005259 measurement Methods 0.000 claims description 23
- 239000000203 mixture Substances 0.000 claims description 12
- 239000003990 capacitor Substances 0.000 claims description 7
- 230000003595 spectral effect Effects 0.000 claims description 6
- 238000012795 verification Methods 0.000 claims description 6
- 238000004458 analytical method Methods 0.000 claims description 4
- 230000000694 effects Effects 0.000 claims description 3
- 238000012544 monitoring process Methods 0.000 claims description 3
- 238000003745 diagnosis Methods 0.000 claims description 2
- 238000012423 maintenance Methods 0.000 claims description 2
- 238000009434 installation Methods 0.000 claims 1
- 238000004088 simulation Methods 0.000 claims 1
- 238000010200 validation analysis Methods 0.000 abstract 3
- 230000009466 transformation Effects 0.000 abstract 1
- 238000012360 testing method Methods 0.000 description 15
- 230000002349 favourable effect Effects 0.000 description 8
- 230000003287 optical effect Effects 0.000 description 8
- 230000009102 absorption Effects 0.000 description 4
- 238000010521 absorption reaction Methods 0.000 description 4
- 238000007689 inspection Methods 0.000 description 4
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 description 4
- 239000000470 constituent Substances 0.000 description 3
- 230000001419 dependent effect Effects 0.000 description 3
- 230000005855 radiation Effects 0.000 description 3
- 238000002716 delivery method Methods 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 230000003203 everyday effect Effects 0.000 description 2
- 230000000737 periodic effect Effects 0.000 description 2
- 230000003679 aging effect Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 238000011109 contamination Methods 0.000 description 1
- 150000008282 halocarbons Chemical class 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 230000002045 lasting effect Effects 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 238000004092 self-diagnosis Methods 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Chemical compound O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
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- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/27—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands using photo-electric detection ; circuits for computing concentration
- G01N21/274—Calibration, base line adjustment, drift correction
- G01N21/276—Calibration, base line adjustment, drift correction with alternation of sample and standard in optical path
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- G01N21/01—Arrangements or apparatus for facilitating the optical investigation
- G01N21/13—Moving of cuvettes or solid samples to or from the investigating station
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- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
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- G01N21/27—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands using photo-electric detection ; circuits for computing concentration
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- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
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- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
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- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
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Abstract
The invention relates to a method for operating a FTIR (Fourier transformation infrared) spectrometer, wherein a validation/calibration of the spectrometer is carried out in cyclically recurring intervals in that by way of at least two temporarily available gases a reference spectrum with a zero gas and also an absorption spectrum with a calibration gas are recorded. The invention further relates to a spectrometer according to the preamble of the patent claims 1 and 8. In order to achieve that at each site of use and at any time a calibration or validation of the spectrometer can be carried out, the invention proposes to use so-called substitute gases during the validation of the spectrometer as gas components, said substitute gases only simulating the actual measured gas component with respect to the metrological properties.
Description
Technical field
The present invention relates to method of operating and FTIR spectrometer itself according to FTIR (Fourier transform infrared) spectrometer of claim 1 and 8 preambles.
Background technology
The FTIR spectrometer is the infrared spectrometer with the computing method work of Fourier transform.This spectrometer is not based on the work of specific absorption spectral line, but writes down the spectrum of whole wavelength coverage and obtain information about the absorption on observed frequency spectrum or the wavelength spectrum (Wellenlaengenspektrum) by means of the spectrometer function (Spektrometerfunktion) of mathematics thus.Carry out stoichiometry (chemometrisch) analysis according to the distribution that is obtained then, and corresponding gas componant is distributed in distribution.Therefore, can measure a plurality of gas componants simultaneously with the FTIR spectrometer.
For by above-mentioned all frequency ranges, use to have the movably interferometer structure work of mirror, for example Michelson (Michelson) interferometer structure.
For device-dependent (geraetebedingt) drift that the change of for example eliminating by transport property causes, must periodic calibration and checking.Only in this way just can guarantee the reliability of measurement result.For easy-to-handle gas componant, such as CO or CO
2, this may be simple.But in general, the FTIR spectrometer also is interested for reluctant gas.This comprises for example NH
3, HCI, HF, H
2O.
But the advantage of FTIR spectrometer is to measure a plurality of gas componants simultaneously.Therefore, this spectrometer especially also is suitable for emission measurement (Emissonsmessung).Usually carry out the inspection of spectrometer every day.
The inspection of calibration data (checking) is carried out with two steps at present usually: the periodic logging that carries out baseline spectrum with short interval (normally every day) with zero gas (Nullgas) (outside air after normally purifying).Come the variation of the transport property of bucking-out system with this baseline spectrum.The variation of transport property for example can be caused by the variation of the variation of the pollution in the optical path, radiation power, detector or by the contamination of measuring unit.The compensation at zero point depends on that wavelength ground carries out, and therefore proofreaies and correct for all constituents at zero point simultaneously.
Is that all constituents carries out the regular checking (inspection) of reference point and also calibrates under possible situation with longer interval (normally jede Woche to annual) with test gas.Easy to handle gas, such as CO, CO
2, NO can be calibrated with the test gas in the test gas bottle under the situation of not additional aid.For the composition that is difficult in the test gas bottle, handle, such as H
2O or HCI, the service test gas generator replaces the test gas bottle.But such processing is difficulty very, and almost can not carry out in some places to use of spectrometer.
The checking of reference point or calibration may be performed under the high situation of technology and time cost, especially when such as H
2When the such gas of O or HCI must be calibrated.Its reason for example is:
-additional technical equipment is installed, such as the test gas generator
-for HCI and H
2The adjusting time that O is long
The calibration that the wrong concentration of-carburetor may lead to errors.
Therefore the checking of reference point and/or calibration can only be undertaken by trained expert.
Therefore, reference point only is examined with the long time interval, does not promptly have the checking of reference point at interval for long measurement.This causes the mistake of concentration to show that risk increases.
US 5,777,735 disclose so a kind of method and apparatus, wherein as other known methods, at gas componant to be measured separately equipment is calibrated in the following manner, promptly the corresponding gas of respective pure form is presented from hold the air-capacitor device as calibration gas.For majority of gas, this is too expensive.
Summary of the invention
Therefore, technical matters to be solved by this invention is further to improve such method and spectrometer, makes in any place to use, can carry out the calibration and the checking of spectrometer at any time.
According to the present invention, for such method, this technical matters is to solve by the feature in claim 1 characteristic.
Other preferred implementations of the method according to this invention provide in dependent claims 2 to 7.
For such spectrometer, according to the present invention, this technical matters is to solve by the feature in claim 8 characteristic.
Other favourable embodiments provide in all the other dependent claims.
The core of the present invention aspect method be, when the checking spectrometer, as to the additional of actual measurement composition or substitute, can also select to cover the easy to handle place of gas composition of the whole spectral limit of spectrometer.For measuring such as HCI, HF, NH
3Reluctant other application scenarios like this, advantageously: can avoid following situation with the method according to this invention, promptly for effectively checking or calibration, above-mentioned gas must be provided with high-purity as test gas.In contrast, use easy-to-handle gas to be used for checking as an alternative, these easy-to-handle gases roughly produce absorption effect in the scope of " difficulty " gas, almost as representative.Thereby, if actual measurement gas for calibrate must with highly purified form and accurately concentration provide, compare with actual measurement gas as checking or this place of gas of calibration gas and be easier to significantly handle.Wherein in the following place of gas that is called as, place of gas obviously is not to be aggressive (aggresiv) or be difficult to like that handle as those gases that it should be represented.Whole checking and calibration become simpler thus.
In another favourable embodiment, the mixed gas that is made of a plurality of place of gas is used to checking, and these a plurality of place of gas cover the sub-range of whole measurement spectrum respectively.By this way, the place of gas that is used for calibrating can be introduced into mixed gas, and this has been chemically adventurous with the actual gas composition.In this way, can in a step, verify the complete spectrum scope of spectrometer immediately.
In another favourable embodiment, so a plurality of place of gas are introduced in the calibration/verification mixed gas, make these place of gas cover the whole spectral limit of spectrometer.
In another favourable embodiment, also monitor the intensity in the checking/calibration steps that uses zero gas, thereby and pass through interpolation and store whole spectrum as benchmark.
In another favourable embodiment, place of gas separately, promptly hold the air-capacitor device from difference, perhaps mixed gas holds the air-capacitor device by single valve control device (Einzelventilansteuerung) from one and is automatically presenting to measuring vessel (Messkuevette) in the checking/calibration steps automatically as an alternative, carries out then and verifies accordingly or calibration steps.Therefore, carry out verification step with the simple and effective way Automatic Cycle.
In another favourable embodiment, determined checking or calibration value are stored in the self-adapting data district, wherein can be as required according to this Data Base Analysis checking/calibration history, so that therefrom obtain the diagnosis of the maintenance state of relevant spectrometer where necessary.
In the end in favourable embodiment, place of gas separately or as an alternative mixed gas is closed, promptly is enclosed in the calibrated vessel (Kalibrierkuevette) and in order to carry out checking/calibration steps, this calibrated vessel changes in (einschwenken) light path automatically, produces from light path again then.
For the FTIR spectrometer, core of the present invention is: such gas is used as the calibration means, promptly this gas only is the representative of actual measurement gas with regard to the assimilation effect in the spectrometer with regard to it, and be stored in and hold in the air-capacitor device, and can automated serial ground when automatically starting calibration or proof procedure one by one or be incorporated into as mixed gas in the light path of spectrometer.
In the favourable embodiment according to spectrometer of the present invention, gas can be introduced in the measuring vessel of spectrometer by means of the automatic valve control device.Therefore, calibration process can be started automatically, and gas is introduced into.
In an alternate embodiments, gas can and can produce again after calibration/verification in the one or more light paths that change spectrometer in gas is filled the calibrated vessel of rear enclosed automatically over to automatically.Therefore, no longer need gas storage.
Description of drawings
Structure at the method according to this invention and spectrometer shows the present invention in the accompanying drawings, and following detailed description the present invention.
In the accompanying drawing:
Fig. 1 shows the principle structure with FTIR spectrometer rotatable or movably calibrated vessel.
Fig. 2 shows the control of calibration.
Fig. 3 shows the spectrum with guide's composition (Leitkomponent) (representative).
Fig. 4 shows the division of spectrum in the zone.
Embodiment
Fig. 1 illustrates the principle structure of FTIR spectrometer, and it for example is arranged on the Michelson interferometer.From radiation source 5, generate parallel light beam by means of first optical system 4 by expansion (Aufweitung), parallel light beam is fallen the semitransparent mirror 3 as beam splitting equipment.Have fixed wave length and the frequency location (monochromatic with relevant) of light drop on now on the fixing mirror 1 and also are reflected there.Other beamlets pass mirror 3 as the crow flies, and by the direction of mirror 2 reflected back mirrors 3 movably, these two beamlets interfere with each other at Jing3Chu now.This interference at this by controllably being handled along optical axis moving lens 2.Begin therefrom, interference light transmission measurement container 8, wherein measurement gas is directed by this measuring vessel.By means of interferometer, measuring vessel, and point-device adjusting of effective frequency position of therefore hitting the light beam of measurement gas have been realized hitting.Therefore, can gather complete spectrum at the detecting device place, and the absorptivity when being not only fixed frequency.For irradiating and detecting device optimally, the light beam of expansion is focused again by second optical system 6, promptly focuses on the yardstick of detecting device.
Measuring vessel air inclusion inlet A and gas vent B, and be introduced into to write down with measurement gas and measure spectrum, again it is drawn then.
In order to carry out according to calibration steps of the present invention, being controlled at this does not now have the valve control device that further shows, and calibration gas is directed or blows and dash by container 8, so that the measurement gas that will measure by valve commutation introducing after calibration.
In another alternative this illustrate, wherein the duration of calibration or checking, calibration gas is being changed in the light path before the detecting device 7 or before optical system 6 by means of calibrated vessel 9.Then, calibrated vessel produces from light path again.
Wherein important will point out, calibrated vessel is not filled being calibrated measured measurement of correlation gas or measurement gas composition in the part at this of spectrometer, but is filled place of gas or alternative mixed gas to represent this measurement of correlation gas or these measurement gas compositions.Therefore, on the spectral limit of spectrometer, for example use SO
2, CO
2, N
2O or methane is gas as an alternative, promptly as representative, rather than very thorny gas componant HCI, HF, NH
3Deng.It is obviously more expensive that the latter is used to calibrate with respective pure form.On the contrary, the place of gas of replacement used according to the invention has just been simplified calibration/verification significantly, because these described alternative compositions can obviously more easily be handled.They are handled so easily, to such an extent as to they are not to calibrate in gas delivery method, now also can handle in airtight calibrated vessel.This is in the past with HCI or HF or even use water vapor H
2O is impossible.
When using calibrated vessel, each gas can be enclosed in the calibrated vessel equally respectively, and can alternately change over to a kind of chopper of form, perhaps the mixed gas of a plurality of place of gas in the gas delivery method, using a common calibration container 9.
Replace changing motion over to, calibrated vessel also can change over to rectilinear motion certainly.
Fig. 2 shows the control according to FTIR of the present invention on principle.Wherein, carry out the manipulation of light source 5 (laser instrument) and detecting device 7 by control module 10.Time control unit 11 triggers calibration process in adjustable time or by clear and definite control signal.For this reason, control mirror 2, light source 5 and detecting device 7 now in phase, and control changing over to or moving and handle of calibrated vessel 9 for this reason in phase, and therefore baseline spectrum is recorded and is stored in the self-adaptation storage unit 12.In addition, storage unit 12 also have the time distributively record data additionally can discern possible aging effect Analysis thus as historical data.Thus, except pure calibration, also carry out the lasting self diagnosis of spectrometer.
Replace changing over to or moving of control calibrated vessel, also can be controlled at the valve control device that is used to present place of gas in the carrying method in phase, so that by using above-mentioned place of gas also to carry out calibration in this mode.
Fig. 3 shows, and replaces the test gas task for all the components, how to verify (inspection) by the test mixed gas that is made of a plurality of place of gas.Place of gas can all be mixed together in the test gas bottle, and stable on a long time interval.Place of gas also can be to measure composition, for example SO
2Or CO
2But, alternatively or additionally, also can use the gas that in different wavelength range, has a plurality of absorptions, for example stable halogenated hydrocarbon or N
2O and CO
2Ideally, place of gas covers the whole spectral limit of spectrometer.
For example, can use following place of gas for this reason.
-long-wave limit is for example used SO
2
-intermediate range is for example used CO
2
-shortwave scope is by methane and N
2O
How additionally Fig. 4 shows the intensity of monitoring criteria spectrum.Therefore, also monitor the wavelength coverage that not replaced gas covers.
If when the checking spectrometer, do not occur the variation of place of gas or each scope of baseline spectrum now, the variation at zero point does not appear, and then do not exist residue to measure the variation of composition (for example HCI or HF) yet.
Opposite with the checking/calibration of service test gas generator, the end of whole process can be by robotization.That is, be used for the zero gas of baseline spectrum and place of gas the test mixed gas can by solenoid valve such computer control as described be stopped.The result can be analyzed automatically, and can trigger warning where necessary.Under than the situation of low deviation, also can trigger warning.
Storage to the checking outcome history can be used as the basis that is used for the continuous mass monitoring.In addition, can store the spectrum of guide's composition and reference value, as previously mentioned.
Alternatively, also can not use the test gas bottle with place of gas constituents mixt fully, method is: be enclosed in the calibrated vessel to the place of gas stable components.Replace test gas task, so calibrated vessel changes in the optical path as mentioned above circularly by solenoid valve.
Reference numerals list
1. the mirror of fixing
2. mirror movably
3. translucent mirror/beam beam splitting equipment
4. the optical system of expanding
5. radiation source
6. the optical system that focuses on
7. detecting device
8. measuring vessel
9. calibrated vessel
10. control device
11. time-controlling arrangement
12. self-adapting data storer
A measurement gas inlet
The outlet of B measurement gas
Claims (10)
- The method of operating of (1.FTIR fourier-transform infrared) spectrometer, wherein at least two gases that temporarily provide had both write down the baseline spectrum of use zero gas, also record uses the absorption spectra of calibration gas by using, carry out the checking/calibration of described spectrometer with the interval that circulation repeats, it is characterized in that, when the checking spectrometer, use so-called place of gas as gas componant, the measurement gas composition of wherein said place of gas only simulation reality with regard to the measuring technique characteristic.
- 2. method according to claim 1 is characterized in that, the mixed gas that is made of a plurality of place of gas is used to checking, and wherein said place of gas covers the subregion of whole measurement spectrum respectively.
- 3. method according to claim 2 is characterized in that, introduces so a plurality of place of gas in introducing the calibration/verification mixed gas, makes these place of gas cover the whole spectral limit of spectrometer.
- 4. according to each described method in the aforementioned claim, it is characterized in that also the intensity of baseline spectrum in the checking/calibration steps of zero gas is used in monitoring, thereby and by interpolation, whole spectrum is stored as benchmark.
- 5. according to each described method in the aforementioned claim, it is characterized in that, described place of gas separately, promptly hold the air-capacitor device from difference, perhaps hold the air-capacitor device from one and automatically presenting to measuring vessel in the checking/calibration steps automatically, carry out corresponding checking or calibration steps then by single valve control device as mixed gas.
- 6. method according to claim 5, it is characterized in that, determined checking or calibration value are stored in the self-adapting data district, wherein can be as required according to this Data Base Analysis checking/calibration history, so that therefrom obtain the diagnosis of the maintenance state of relevant spectrometer where necessary.
- 7. according to each described method in the aforementioned claim, it is characterized in that, described place of gas separately or as an alternative mixed gas is closed, promptly is enclosed in the calibrated vessel, and in order to carry out checking/calibration steps, this calibrated vessel changes in the light path automatically, produces from light path again then.
- 8. the FTIR spectrometer that has checking and/or calibrating installation, be used for verifying circularly and/or calibrating the measurement spectrum of FTIR spectrometer, it is characterized in that, such gas is used as the calibration means, promptly this gas only is the representative of actual measurement gas with regard to the assimilation effect in the spectrometer with regard to it, and be stored in and hold in the air-capacitor device, and can automated serial ground when automatically starting calibration or proof procedure one by one or be incorporated into as mixed gas in the light path of spectrometer.
- 9. FTIR spectrometer according to claim 8 is characterized in that, described gas can be introduced in the measuring vessel of spectrometer by means of the automatic valve control device.
- 10. FTIR spectrometer according to claim 8 is characterized in that, described gas can and can produce again after calibration/verification in the one or more light paths that change spectrometer in gas is filled the calibrated vessel of rear enclosed automatically over to automatically.
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
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DE102007056345A DE102007056345B3 (en) | 2007-11-22 | 2007-11-22 | Method for operating fourier transformation infrared-spectrometer, involves utilizing residual gases as gas components in each case during validation of spectrometer, which simulate actual measuring gas component |
DE102007056345.2 | 2007-11-22 | ||
PCT/EP2008/009854 WO2009065595A1 (en) | 2007-11-22 | 2008-11-21 | Method for operating an ftir spectrometer, and ftir spectrometer |
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CN101918814A true CN101918814A (en) | 2010-12-15 |
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CN2008801170089A Pending CN101918814A (en) | 2007-11-22 | 2008-11-21 | Method for operating an FTIR spectrometer, and FTIR spectrometer |
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US (1) | US20100282958A1 (en) |
EP (1) | EP2215454A1 (en) |
CN (1) | CN101918814A (en) |
DE (1) | DE102007056345B3 (en) |
WO (1) | WO2009065595A1 (en) |
Cited By (5)
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CN103403529A (en) * | 2010-12-23 | 2013-11-20 | Abb股份公司 | Optical gas analyser device having means for calibrating the frequency spectrum |
CN103635785A (en) * | 2011-02-15 | 2014-03-12 | 勒克思马克斯科技公司 | A fully integrated complementary metal oxide semiconductor (CMOS) fourier transform infrared (FTIR) spectrometer and raman spectrometer and method thereof |
CN108072624A (en) * | 2016-11-18 | 2018-05-25 | 天津邦纳科技有限公司 | A kind of method that amount of nitrogen oxides chemical sensor and spectrometer mutually verify |
CN108072623A (en) * | 2016-11-18 | 2018-05-25 | 天津邦纳科技有限公司 | A kind of method that content of sulfur dioxide chemical sensor and spectrometer mutually verify |
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EP2635902B1 (en) * | 2010-11-01 | 2018-12-12 | Koninklijke Philips N.V. | A method of calibrating an air sensor |
US8467996B2 (en) | 2011-02-09 | 2013-06-18 | Jorge E Perez | Spectral analysis operating system |
RU2571185C2 (en) * | 2011-08-19 | 2015-12-20 | ФОСС Аналитикал А/С | Method to compensate for amplitude drift in spectrometer and spectrometer realising specified method |
DE102013101610B4 (en) * | 2013-02-19 | 2015-10-01 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Apparatus and method for remote detection of a non-infrared active target gas |
DE102013005997B3 (en) * | 2013-04-08 | 2014-05-15 | Abb Technology Ag | Optical gas analyzer device for use with industrial chimney of waste-incineration plant, has processing unit determining gas concentration of total carbon contained in measurement gas other than analyzing pollutant components |
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Family Cites Families (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE4128912C2 (en) * | 1991-08-30 | 1995-06-22 | Deutsche Forsch Luft Raumfahrt | Method and device for the calibration of spectroradiometers |
US5777735A (en) * | 1996-09-30 | 1998-07-07 | Minnesota Mining And Manufacturing Company | In situ analysis apparatus |
CA2267558C (en) * | 1998-04-10 | 2005-09-13 | Her Majesty The Queen, In Right Of Canada, As Represented By The Ministe R Of National Defence | Fourier-transform spectrometer configuration optimized for self emission suppression and simplified radiometric calibration |
US7535006B2 (en) * | 2003-06-09 | 2009-05-19 | Canberra Albuquerque, Inc. | Gaseous uranium hexafluride isotope measurement by diode laser spectroscopy |
JP4591105B2 (en) * | 2004-05-31 | 2010-12-01 | 横河電機株式会社 | Calibration method |
DE102004031643A1 (en) * | 2004-06-30 | 2006-02-02 | Abb Patent Gmbh | Non-dispersive infrared gas analyzer |
US7598494B2 (en) * | 2007-01-30 | 2009-10-06 | Airgas, Inc. | Automated FTIR gas analyzer |
-
2007
- 2007-11-22 DE DE102007056345A patent/DE102007056345B3/en active Active
-
2008
- 2008-11-21 EP EP08851951A patent/EP2215454A1/en not_active Withdrawn
- 2008-11-21 WO PCT/EP2008/009854 patent/WO2009065595A1/en active Application Filing
- 2008-11-21 CN CN2008801170089A patent/CN101918814A/en active Pending
-
2010
- 2010-05-21 US US12/784,757 patent/US20100282958A1/en not_active Abandoned
Cited By (7)
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CN103403529A (en) * | 2010-12-23 | 2013-11-20 | Abb股份公司 | Optical gas analyser device having means for calibrating the frequency spectrum |
CN103403529B (en) * | 2010-12-23 | 2015-07-22 | Abb股份公司 | Optical gas analyser device having means for calibrating the frequency spectrum |
CN103635785A (en) * | 2011-02-15 | 2014-03-12 | 勒克思马克斯科技公司 | A fully integrated complementary metal oxide semiconductor (CMOS) fourier transform infrared (FTIR) spectrometer and raman spectrometer and method thereof |
CN103635785B (en) * | 2011-02-15 | 2016-11-02 | 勒克思马克斯科技公司 | Integrate CMOS-FTIR measures and Raman measures spectrogrph and method thereof |
CN108072624A (en) * | 2016-11-18 | 2018-05-25 | 天津邦纳科技有限公司 | A kind of method that amount of nitrogen oxides chemical sensor and spectrometer mutually verify |
CN108072623A (en) * | 2016-11-18 | 2018-05-25 | 天津邦纳科技有限公司 | A kind of method that content of sulfur dioxide chemical sensor and spectrometer mutually verify |
CN112540053A (en) * | 2020-09-27 | 2021-03-23 | 杭州春来科技有限公司 | Open type gas detection device |
Also Published As
Publication number | Publication date |
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WO2009065595A1 (en) | 2009-05-28 |
EP2215454A1 (en) | 2010-08-11 |
DE102007056345B3 (en) | 2009-01-02 |
US20100282958A1 (en) | 2010-11-11 |
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